Compass system



Jan. 19, 1954 w. H. KLlEvER COMPASS SYSTEM 3 Sheets-Sheet l Filed Dec. 26, 1947 nventor W/7L00 h. /fL /EVE/f Gttorneg Jan. (19, 1954 Filed Dec. 26, 1947 W. H. KLIEVER COMPASS SYSTEM 3 Sheets-Sheet 2 Bnventor (Ittorneg Jan- 19 1954 w. H; KLIEVER 2,666,268

COMPASS SYSTEM Filed Dec. 26. 1947 3 Sheets-Sheet 3 Snventor Patented Jan. 19, y 1954 UNITED STATES sans FATENT OFFICE COMPASS SYSTEM Application December 26, 1947, Serial No. 793,819

17 Claims.

This invention relates to the field of magnetic Compasses, and more particularly to remote indicating or controlling compass systems in which the compass is a cathode ray tube whose beam is deflected by the earths magnetic iield.

The use of a cathode ray tube to indicate the direction of the earths magnetic field and hence to act as a compass is known. It has been proposed to visually observe the location of the trace on the cathode ray screen as an indication of compass direction, and also to adjust the physical position oi the cath-ode ray tube so as to bring the trace to a predetermined position on the screen, and to interpret the position taken by the tube as an indication of the direction of the earths magnetic eld. It has further been proposed to maintain the cathode ray tube with its axis vertical, and to actuate a remote indicator in accordance with the deflection oi the cathode ray beam. The present invention is an improvement on known systems, and is of the type last described. It is accordingly an object of the invention to provide an improved compass system embodying a cathode ray compass and a remote motor actuated indicator.

It is another object of the invention to provide an improved angle repeating system in which the operation of the system includes as steps deteri ming the components of the angle along a pair of axes and subdividing the components in proportion to components oi a second angle along a second pair of axes, so that the subdivisions are equal when the two angles are equal.

It is another object of the invention to provide a new resistance unit in which voltages proportional to the components of an angle may be subdivided as just described.

Another object of the invention is to provide an improved aircraft compass system in which a directional gyroscope is slaved to a cathode ray compass by means of the above described angle repeating system.

Yet another object of the invention is to provide a cathode ray compass system in which the effects or" noncircularity of the electron beam and of nonuniiorinity in amplifying and rectifying components are minimized by a degenerative feedback component effective on the deflection of the beam.

A still further object of the invention is to provide a system as described above in which the low level alternating output voltages of the cathode compass are converted to higher level unidirectional voltages ior the feedback component, and then part reconverted to alternating voltages for operating an alternating current motor actuating the remote indicating means.

Various other objects, advantages, and features of novelty which characterize my invention are pointed out with particularity in the claims annexed hereto and forming a part hereof, or will become apparent from the reading of the speciiication. However, for a better understanding of the invention, its advantages, and objects attained by its use, reference should be had to the subjoined drawing, which forms a further part hereof, and to the accompanying descriptive matter, in which I have illustrated and described certain preferred embodiments of my invention. In the drawing:

Figure 1 is a schematic showing or" a complete compass system according to the invention;

Figure 2 is a schematic showing of a simplified inodication of the complete system;

Figures 3, 4 and 5 are views illustrative of certain details 'of the invention;

Figure 6 is a schematic showing of a resolver suitable for use in the practice of my invention;

Figure '7 is a schematic showing of an improved resolver adapted for use in the practice of my invention; and

Figure 8 is a diagram showing certain voltage relations occurring in the structure of Figure 1.

Construction of the system of Figure 1 Referring now to Figure l, there is illustrated a cathode ray tube it functioning as a compass and energized from a power supply Il. Electrical outputs from the cathode ray tube are impressed by transformers l2 and i3 upon a pair of electronic units ld and I5 each of which comprises an amplier and a phase sensitive rectiiier of the type shown in Upton Patent 2,423,534 issued July 8, 1947. The outputs of units ifi and l5 are conducted to recentering coils it and il associated with Icathode ray tube i t, and are also made use of to actuate instruments for performing indicating and control functions in accordance With the response of the compass to the earths magnetic field. One or these instruments is a ratio meter indicated at 2t, another is a motor actuated indicator 2|, and a third is a directional gyroscope 22.' The outputs of the electronic units are supplied to indicator 2l through a resolver 23, 4which will be described in more detail later, and a phase sensitive ampliiier Since the output of resolver 23 is a unidirectional voltage,

interrupter 2l is provided to convert this voltage to an alternating one. In a similar fashion directional gyroscope 22 is energized with the outof electronic units it and i5 through a resolver d phase sensitive amplifier 26, a 2S being provided to perform n as actuating a control member eifective to control the course of f the compass system, or to perferm such other functions as may be considered desirable. The various components referred to above will now be described in more complete detail.

Cathode ray tube l is shown to comprise an evacuated envelope 3D enclosing a plurality of electrodes to which electrical connection may be made from outside the tube by suitable conductors passing through the envelope. rlhus there is shown at 3i a heater filament for raising the temperature of a cathode 32 to a point at which it is thermoemissive. A control electrode or grid is provided for controlling the flow of electrons from the cathode, and a plurality of apertured focusing and accelerating electrodes 34, and are also provided. Elements 3l to 36 inclusive comprise an electron gun which functions to direct a beam of electrons 31 along the longitudinal axis 38 of the tube. Because the apertures in electrodes 34, 35 and te are cirn cular, the cross section of the beam is also cirn cular, and since the apertures are axially aligned, the axis of the beam is very nearly aligned with the axis of the tube. However, because of the unavoidable manufacturing tolerances, it is impossible to produce in commercial quantity tubes in which the axis or? the beam is exactly aligned with that of the tube. reason pairs of electrostatic deecting plates-n dil and M, and t2 and i3- are provided, so that by the application of suitable voltages therebetween the position of the axis of the beam may be exactly adjusted.

At the end of cathode ray tube l@ remote from the electron gun there are located a plurality of target plates M, 4B and 41. These plates are substantially in the same plane, and taire the form of mutually insulated circular quadrants. The plates are arranged in pairs which are bilaterally symmetrical about axes which are mu tuallv perpendicular.y and which are also perpendicular to the axis of the tube.

External to the tube are mounted the recentering coils le and l1, each coil being preferably composed of two coaxial sections, one mounted on either side of the tube. The axis 50 of coil i6 is in a plane perpendicular to the axis about which each of plates 46 and 41 is symmetrical and is parallel to deilecting plates t2 and 43. The axis 5i of coil I'! is perpendicular to the axis about which each of plates 44 and 45 is symmetrical, and is parallel to deflecting plates il and 4|.

The inner surface of tube l0 is coated with an electrically conducting material such as carbon deposited. fromv a colloidal suspension, as indicated at 52.

lTube Il) is received within a mounting ring 53, which is pivoted by diametrically opposite pins till to a Cardan ring 55. The axis of pins lid is parallel to the axis 5| of deflecting coil Il, and Cardan ring 55 is pivotally supported vby means not shown in a member rigidly connected to the aircraft or other vehicle in which the compass is mounted: the axis of pivotal movement between Cardan ring 55 and the external support is par= allel to axis til) of recentering coil lli. By reason of the location of mounting ring 53 spaced trom For this the center of gravity of the tube, the latter is pendulously mounted so that its longitudinal axis is parallel to the direction of apparent gravity. Horizontal accelerations o the craft cause departure of the tube axis from true vertical, but these accelerations average out to zero, so the average position of the tube axis is true vertical.

The compass tube is preferably installed in the vehicle so that the heading of the vehicle coincides with axis 59, as indicated by arrow 59.

The structure thus far described functions, when suitably electrically energized and in the absence of any external magnetic field, to direct a beam of electrons 31 along the vertical axis of the tube so that it impinges upon the target plates, the center of the beam accurately coinciding with the center of the target plate assembly, and the outline of the `beam being a circle, so that the areas of the several plates impinged by the beam are all egual, and equal target currents flow in circuits presently to be If the heading of the craft is due north, the earths magnetic field acts upon t e to delect it from its central position. Since the tube is pendulously mounted so that its axis is nor mally vertical, the vertical component of the earths magnetic iield is not eiiiective on the beam, but its horizontal component is effective, whether in the northern hemisphere or in the southern hemisphere, to deflect the beam toward the east. The magnitude of the horizontal component of the earths magnetic field, and hence the amount of deiiection of the beam varies with latitude, being greatest at the magnetic equator.

When the beam is deflected from its center position the impinged areas of the several target plates are no longer equal, and unequal target currents now.

Figure 3 shows the target plates as viewed from the electron gun, and in this view the area of the plates impinged by the beam is indicated by the circle 56. It will be observed that the center 51 of the beam is displaced to the east of the center of the target plates, the amount of this displacement being determined by the horiu zontal component of the earths magnetic 'Field at the location of the compass. If the tube is now rotated in azimuth, the center of the beam describes an arc indicated by the dotted circle so that for any position of the tube in azimuth, the relative areas of the plates iinpinged by the beam, and therefore the various target currents, are different. Thus in Figure 3 the areas of plates 44 and 45 impinged by the beam are equal, while the areas of plates t6 and il impinged are unequal, that of plate 41 being the greater. 1f the heading of the craft changes so that it is directed west of north, as shown in Figure 4, by an angle 0, the center of the beam 51 is displaced around the circle 6G to a new position through an angle also equal to 0.

If the radius of circle 60 is suciently small, the diference between the impinged areas of plates 41 and 46 varies as a cosine function of the angle 0, and the difference between the impinged areas of plates 44 and 45 varies as a sine function of 0. While this is not a mathematically exact relation, practical tests have shown that the approximation is sufficiently precise for the present use of the apparatus.

The various electrodes of cathode ray tube I0 are electrically energized with alternating and unidirectional voltages from power supply H, which is shown to comprise a pair of terminals 5! ,and 6,2 energized from any suitable source of having movable sliders 'l1 and 80 respectively.'

Power supply is shown to comprise further potential dividers 8|, 82, 83 and I8f3, a pair of filtering condensers 85 and l86, and a ground connection 81.

Potential divider 8| comprises a winding 90 .and a slider 9| lmovable-with respect thereto. Potential divider 82 comprises a winding 52 and aslider- 93 movable with respect thereto. Sliders 9| and 93 are manually operable unitarily, so that both move to the left or to the right at the same time. Potential divider 33 comprises a winding ,94 and a slider S5 movable with respect thereto. .Potential divider 84 comprises a winding .at and a slider 91 movable with respect thereto. Sliders 95 and 9T are also operable by manual means not shown to move unitarily to the left or to the right Vat the same time.

Potential dividers lil and 82 are provided for the purpose of determining the relative potentials on deflecting plates 42 and 43. 'When sliders .9| and 93 are to the left of their central position, plate 43 is positive with respect to plate 42, and when the sliders are displaced in opposite direction the relative polarity of the plates is reversed. Similarly potential dividers 83 and 84 determine the relative potentials of deiiecting plates 40 and 4| when sliders 95 and -Sl' are 'at the left of their center positions, plate 40 is Ypositive with respect to plate 4|, and the relative polarity is reversed when the sliders are transversed to the right of their central position.

Secondary winding 61 of transformer 65' provides voltage for heater filament 3| of the tube, and secondary winding l and potential divider 'IS combine to maintain grid 33 at a potential, with respect to cathode 32, which alternates about a negative value determined by the position of slider 80, at the frequency of the source sup- ,f

plying alternating voltage to terminals and 62: the amplitude of the modulating voltage is such that grid 33 never becomes positive with respect to cathode 32.

Target plates 44, 45, 46 and 4l, electrodes `34 and 35, and conducting layer 52 are all maintained at ground potential, with respect to which cathode 32 is maintained highly negative, thus bringing about the proper condition for thermal emission of electrons, and their formation into a directed beam is assisted by the presence on electrode 35 of a moderate positive charge compared to that of cathode 32.

The target currents flowing in plates 44 and 45 are compared in transformer I3, which is shown to comprise secondary winding |00 and a primary winding |0| having a center tap |02. Similarly the target currents flowing in plates i6 and 41 are compared in transformer l2, which is shown to comprise a secondary winding |03 rand a primary winding |04 having a center tap |05.

Electronic unit |4 is shown to comprise a pair of input terminals |06 and |01, a pair of output terminals ||0 and and a pair of power terminals 2 and ||3. The input terminals are energized with voltage from transformer I2 in accordance with the difference between the target currents in plates 46 and 4l. Since the voltage output of transformer |2 is exceedingly minute, electronic unit 4 comprises a voltage amplifier: this is followed by a phase sensitive rectifier, so that the output at terminals llt and is a pulsating unidirectional voltage the magnitude of which is determined by the amplitude of the voltage supplied to the input terminals of the unit, and the polarity of which is determined by the phase of that input voltage compared to the voltage supplied at the power terminals ||2 and ||3 of the unit.

Similarly, electronic unit l5 is shown to comprise a pair of input terminals H4' and H5, a pair vof output terminals IIB and a pair of power terminals |20 and |2I. The components of electronic unit I5 are the same as those of unit I4, and there appears at the output terminals ||5 and ||1 of this unit a pulsating unidirectional voltage the magnitude of which varies with the amplitude of the voltage applied to the input terminals of the unit, and the polarity of which is determined by the phase of that alternating voltage. Alternating voltage is provided to power terminals ||2, 3, |20 and |2| from the source connected to terminals 6| and 82.

The pulsating unidirectional output voltage from electronic unit le is impressed across a pair of resistors |24 and 25 having a cci non terminal |2. By of suitable filtering condensers i2?, |38 and is! the alternating compcnents of this pulsating voltage are practically removed, the remaining voltage drop across resistors |24 and |25 being essentially a reversible unidirectional one whose magnitude varies with variation in the difference between the target currents traversing plates and The output from electronic component i5 is similarly impressed acrcss a pair of series resistors |32 and ist having a common terminal |34, and provided with filtering condensers E35 and |37, so that the voltage across resistors |32 and |33 is essentially a reversible unidirectional voltage whose magnitude is determined the dierence between the target currents in plates 4d and 45.

For purposes of definition reference should now be made to Figure 5. This figure illustrates the fact that the components .r and y, along mutually perpendicular axes XX and ci a displacement lcI-l caused by the horizontal component of the earths magnetic eld have the respective values given below, where 41 is the angle between the direction of the movement and the maxis.

=kH cos c (l) and 1I=IcH sin fp (2) For convenience in future referenc plates 45 and All in Figure 1 will be ei as the cosine plates, transformer i2 as target e cosine transformer, electronic unit is as the cosine unit, and the filtered voltage across resistors |25 and l' as the cosine voltage: in every case it will `be understood as an abridgement of wcrding identifying the subject with that component of the earths magnetic field is maximum when the craft is heading north. Similarly the adjective sine will be applied to target plates die and d5, transformer' i3, electronic unit and the voltage appearing across resistors 32 and |33, identifying components which have their' minimum value when the craft is heading north.

Ratio meter 2li if provided is used to give a qualitative indication or change in the heading of the craft from some arbitrarily selected value for which the meter is adjusted to give its central Zero indication. to compare the electrical energization supplied to it from the cosine and sine voltages, and may conveniently be a diierential voltmeter. If an actual ratio meter is used, its indication is directly proportional to the tangent of the angle by which the heading oi the craft departs from the selected heading, since definition the tangent of any angle is the ratio oi its sine to its cosine.

The cosine voltage is applied to recentering coil i6, and the sine voltage is applied to recentering coil il, each a proper sense to return the beam 'toward the center, so to reduce the target current difference which causes the sine and cosine voltages. The gain in the amplifiers of electronic units iii and la is so adjusted as to give sine and cosine voltages of magnitudes which cause currents in coils le and i'i almost sufficient to return beam to its central or no-eld position. This relationship is best illustrated in Figure 3, where, it will be recalled, the craft is assumed to be heading north. The effect oi the voltages fed back to coils it and il, hereinafter referred to as the recentering voltages, is to greatly reduce the size of circle bil about which the center ci the beam to move when the tube is rotated in azimuth, so that it has a smaller value indicated by circle |40. The position of the center oi the beam is indicated by reference numeral and the beam in its new position by reference numeral |42.

The relationships in Figures 3 and i have been greatly exaggerated to malte the showing clearer. ln an actual embodiment of the invention the target plate circle has diameter oi 7/8 of an inch, the diameter of the beam at the target is of an inch, the circle traced by the center or the beam without the recentering coil has a radius of 1/8 or' an inch, and the circle traced by the cen er of the beam with the rebalancing coil has a radius ci about 1/go of an inch. Although the recentering of the beam by this means does in effect comprise a reduction of the sensitivity ci the tube, this is compensated for by the increased accuracy with which the sine and cosine voltages follow their respective trigonometric functions, and by the fact that the disturbing effects of noncircularity of the beam section and non-identity of the electric units on the response of the instrument are greatly minimized.

The sine and cosine voltages are red to a resolver 23 which is shown to comprise a pair of cosine terminals |43 and it, a pair of sine terminals |45 and Mii, a pair or" output terminals |41 and |53, and a driving shaft Ibi. Resolver |23 is shown in detail in Figure 6 to comprise a pair of resistance units |53 and |54 with respect to which there move a` pair of contacting sliders |55 and |56.

Resistance unit teil comprises a pair of resistance members |51 and itil and a pair of electrically conducting members lei and H52. Each of. resistance members |51 and i6@ comprises a nonconducting rod carrying a winding of fine insulated wire. Members l'l and |69 are suitably mounted to form the opposite sides of a The instrument 'functions 8 rectangular frame, of which members ibi and |62 suitably mounted comprise the other two sides. The ends of the wires comprising the windings are soldered to the conducting members to complete a closed electrical circuit, and the insulation is removed from the winding along a line so that electrical contact may be made to the winding at any point. In addition, the solder connecting the wire to the conducting member is carried along the winding toward` the center thereof so that the angles subtended by the windings, at a central pvot, are both and the remaining angular space is equally divided. The windings, the conducting mem-bers, and the solder are arranged to be substantially in a common plane, and thus comprise arsquare with two resistance arms and two conducting arms. Slider |56 is pivoted at the center oi the square, and is resiliently maintained in continuous contact with the resistance member with which it cooperates to comprise what will be referred to as the cosine resistor.

Slider |55 cooperates with the resistance unit |53 to comprise a sine resistor. The construction of resistance unit |53 is in every respect similar to that of unit |52: it is shown to comprise resistance members |63 and |64 and conducting members |65 and |66, mounted to form a square for contact by slider |55. Sliders |55 and |56 are mutually insulated, and are simultaneously operated by shaft |5|. The resistance units are so mounted with respect to the sliders that when slider |56 is midway along resistance member |51, slider |55 is midway along conducting member |66: this will be referred to as the normal or zero setting of the resolver.

Suppose a voltage proportional to the cosine of an angle 0 is impressed between terminals |43 and |44 so that they are respectively positive and negative, compared to a reference point, by equal amounts, and suppose a voltage proportional to the sine of the same angle 0 is likewise applied between terminals |45 `and |46 so that they are respectively positive and negative by equal amounts, with respect to the same point. Let the angle by which sliders |55 and |56 are displaced from the zero position be e, a counterclockwise rotation being considered positive. Then for values of less than 45, slider |55 is at a potential, with respect to the reference point, of i sin 0 and slider |56 is at a potential with respect to the reference point of cos 0 tan qi 2 'I'he potential diierence V between the sliders is given by the equation *sin 0 cos 0 tan b 2 2 When =0, the second term on the right becomes and siider'lst is at a potentiai'with respect to the reference point of y cos 0V The potential. difference V between the sliders is now given by the equation and becomeszero when 0 equals gb.

It can be shown that for any positive or negative value of 0, a position of sliders |55 and |55r tendency to instability at values for angle 4S- of inultiples of and when gb is greater than 0 the voltage difference between the sliders is always of the opposite polarity Ito that when qb isfless than 0. The output of resolver 23 is thus a unidirectional voltage the magnitude of which is zero when the shaft |52 is in angular agreement with the direction of the field.

Interrupter 21 is shown in Figure 1 to coinprise an energizing winding |10, a movable contact |1|, and a pair of xed contacts |12' and |13 to which are respectively connected terminals |41 and |56 of resolver 23. Winding |15 is energized with alternating voltage of the selected frequency from the secondary winding |14' of a transformer |15 of which the primary winding |16 is energized from terminals 8| and 52 connected to the A. C. source. Movable contact |1| vibrates at the frequency of the alternating voltage supplied to the energizing Winding, andv makes contact first with fixed Contact |12 andl then with iixed contact |13. Neglecting transients, the voltage on movable contact |1| is shown as the square wave |8| in Figure 8, and has the same period as the source energizing the vibrator. It is assumed in Figure 8 that slider |55 of resolver 23 is positive with respect 'A to slider |56: accordingly the upper limits of the wave occur when movable contact |1| engages xed contact |12, and the lower limits of the curve occur when movable contact |1| engages xecl contact |13. If the relative polarity of sliders |55 and |56 reverses, the phase of the square wave ISI also reverses, while if sliders |55 and |56 are at the same potential, square wave 8| becomes a straight line. The voltages are all measured with respect to the reference point, which is indicated at |82 in Figure 8. Movable contact |1| is connected to the refer-l ence point through a blocking condenser |83 and the winding |84 of a voltage divider |85 having a slider |85. The reference point is maintained at ground potential by a ground connection |88.

As is well known to those skilled in the art, a voltage having the wave shape of curve |8| is comprised of a unidirectional component, indicated at |81, a rst alternating component of the fundamental frequency, indicated at |90, and harmonic components having frequencies which are integral multiples of the fundamental frequency. The magnitude of the unidirectional' component varies with angle 0, and may be either amplifier lis of a well known -type in which the output terminals areenergized in a iirst fashion if tne voltages on the power and input terminals are in phase, and in tne opposite i'asnion if the voltages are out of phase: alternating components of the input voltage differing materially rroinftne power frequency are Without substantial effect on the amplifier.

` pitted cauti.

A spilt phase motor zoll, which is designed for operation on alternating voltage of the frequency oi the source, is energized from ampliner as' to operate in a first direction when the output terminals of the amplifier are energized intiie iirst iasnion, and in tne opposite direction when the output terminals are energized in the opposite iasnion. lvlotor ou drives shaft liii, winch has been shown to adjust sliders m5 and les ci resolver ze, anu also drives a shaft tail to winch is iasteneu an index zur wnicn is accordingly moved with respect to a iixed index bucn gear reduction, not shown, as is desired may be provided between nictor 2e@ anu snaits lul and` icl, but the gearing must se suon tnat the shaits rotate tniougn equal angles for any given amount of operation of i motor 255.

'ine general functioning of this portion of the system 4will now be apparent. As the cathode ray beam is deflected from a position of equal impingement or' all the target plates, in response to the earths magnetic iield, voltages are impressed on resolvel z3 proportional to the components of the earths magnetic held along the longitudinal and transverse axes of' the craft. 1f the resolver is not so set that its angle from the zero position is the same as the angle of the earths magnetic field from the longitudinal axis of the crai't, fixed contacts |"l2 and |13 are not at the same potential, and amplifier 25 eneigizes motor 25u to operate such a direction as to bring sliders |55 and |56 to the position at which they are at the same potential. 'When this position is reached, operation oi motor 25u stops. Index 22 is set at the North graduation on plate 253 when the resolver is in its .normal position, and the direction oi" operation nais ZilliA and 255, sine terminals 25e and fel,

output terminals 2| and 2H, and a driving shaft 2|2. Resolver 21| is constructed exactly like resolver 23 previously described, and energizes the fixed contacts 2|3 and 2|4 of interrupter 28, which has a movable contact 215 and an energizing winding 216. Movable contact 2|5 is connected to ground through a blocking condenser 241 and the winding 225 of a potential divider 22| having a slider 222, and a portion of the alternating component of the voltage across winding 22d is applied to the input terminals and 22d of the second phase sensitive amplifier zii, which has power terminals 223 and 2m and output terminals 221,23c and 231.

Amplifier 2t energizes a split phase torque motor 232 comprising a portion o1' directional gyroscope 22. The gyroscope includes a mounting within which a rotor 23H spins about an axis Mounting 233 is pivotally supported in a cardan ring 235 for pivotal movement about 'an axis 2st, and cardan ring 233 is in turn mounted pivotally for rotation about a vertical axisrel. A graduated scale 211i) is carried by cardan ring for movement with respect to a fixed index 213i to give indications of azimuth. Similarly a slider 2&2 is carried by cardan ring but insulated therefrom, and engages the winding 21.13 of a potential divider making up control member 2li. By this means there `is provided a control voltage which varies in accordance with change in the heading of the craft, since .slider 232 is stabilized in azimuth by the gyroscope, and winding 243 is fastened to the craft i'or azimuth movement therewith. Drive sliart 212 or resolver 24 is connected to the vertical axis of gyroscope 22, so that the position of the sliders or' resolver 2li is determined by the position in azimuth of the gyroscope.

It is well known that a directional gyroscope gives a much steaciier indication oi' azimuth than does a magnetic compass, for example, because of its comparatively enormous period in azimuth. 'lit is also known, however, that the azimuth indications oi' a directional gyroscope are subject to continuous slow departure from the correct value, so that for accurate navigation the directional gyroscope must be reset frequently in accordance with the indications of a magnetic compass. The causes ci' this precession of the gyroscope away from its original position in space have been discussed in the prior art and this discussion will not be repeated here. rlhe prior art has also suggested the desirability of slaving a directional gyroscope to a magnetic compass, so that the actual azimuth indication will not be subject to violent fluctuations, and yet so that any sustained deviation between the indication or the gyroscope and that of the magnetic compass will be corrected by intentional precession of the gyroscope in azimuth. This precession oi' the gyroscope is accomplished according to the present invention by torque motor 232, which applies torque about axis 236 in one direction or the other according as the energization oi' terminals 22?, 23] and 231 is in a first sense or in the opposite sense. Application of torque around axis 233 results in procession of the gyroscope around vertical axis 23'1, according to well known principles of gyroscopic operation.

The general functioning of this portion of the compass system will now be apparent. As long as the magnetic compass and the directional gyroscope are properly coordinated, the position of the sliders of resolver 24 is so related to the direction of the displacement of the beam of the cathode ray tube that no voltage difference appears between xed contacts 213 and 214, and torque motor 232 is deenergized. Any change in the heading of the craft displaces the beam of the cathode ray tube, but equally displaces the winding of resolver 24 with respect to the sliders, which are stabilized by vgyroscope 22 through shaft 212, and there is still no voltage appearing between fixed contacts 213 and 214. However,

should gyroscope 22 begin to drift in azimuth while the heading of the craft remains the same, the sliders of resolver 24 are moved with respect to their windings, and a voltage difference appears between xed contacts 213 and 214. This is converted to an alternating voltage according to principles previously described, and this in turn energizes torque motor 232 in such a direc. tion as to precess the gyroscope so that the sliders of resolver 24 are returned to a position in which the resolver gives no output voltage, and the azimuth indication of the gyroscope is at the same time corrected so that it is again correlated with the magnetic field indicated by the compass. It will be realized that the torque which torque motor 232 is capable of exerting must be so selected with respect to the inertia of the-rotor spinning at its rated speed that the gyroscope will only follow the average or long term indication of compass, and will not respond to temporary or transient indications. I have found that correction of the position of shaft 212 at 4 per minute is a satisfactory rate of operation for this portion of the system.

Although shown separately for clarity of illustration, potential dividers 81, 82, 83 and 84 are in practice mounted with tube 10. This is for convenience in centering the beam, since actual. field-free space is not easy to establish, while improper centering of the beam causes it to vary in deflection with change in the voltage applied to terminals 63 and 64. The centering process is carried out as follows. The tube without the balancing coils but with the potential dividers fixed thereto is set up in a test fixture with its axis as nearly parallel to the earths magnetic eld as can be estimated, and with test voltages on the various electrodes. The sliders 91, 93 and 95, 9'1 are adjusted until the spot is at the center of target plates 44, 45, 46, 41, as indicated by equal target currents. Itis still possible, however, that the central position of the beam is due not entirely to the centering voltages, but in part to a residual component of the earths magnetic field resulting from imperfect alignment with the beam axis therewith. To obviate this uncertainty, the electrode voltages are all increased sharply by increasing the voltage of the supply. If the beam is actually parallel to the earths eld, this will cause no deflection, but if there is a component of the neld normal to the beam, deflection will result. The process is repeated until no change in the position of the beam takes place. Thereafter the tube may be installed in any desired position and location and connected into the system: any variation in the operating voltage impressed between terminals B3 and 64 will now be ineiective on the deflected portion of the beam.

In setting up the instrument, the cathode ray tube is mounted, in an aircraft for example, so that axis 50 is in a vertical plane parallel to the longitudinal axis, or heading, of the craft: axis 3B is vertical because of the force of gravity acting on the universally mounted pendulous tube. The craft is turned so that its longitudinal axis is in the magnetic meridian. Shaft 212 is uncoupled from the gyroscope 22, whose spinning motor is not energized, and shafts 151 and 291 are uncoupled from motor 200. Terminals 61 and 62 are connected to a source of 400 cycle, volt single phase A. C., and terminals 63 and 64 are connected to a source of 450 volts D. C. sc that terminal 63 is positive.

Energization of terminals 6| and 62 acts through conductors 250 and 25| to energize primary winding 66 of transformer 65, and an alternating voltage is induced in secondary winding 61 by transformer action, and applied to heater lament 3| by conductors 252, 253 and 254: in the embodiment of the invention shown in Figure 1 the filament voltage is 6.3 volts. By this means, cathode 32 is brought into thermoemissive condition.

Target plates 44, 45, 46 and 41 are maintained substantially at ground potential by being connected through circuits traced below to junction point 255, to which is also connected ground connection 81. Since cathode 32 is maintained several hundred volts negative with respect to the target plates, by being connected to junction point 256 between voltage dividers 15 and 1,6, and is heated to thermal emission, target currents making up the anode current of the tube flow yin a plurality of circuits having electron beam 31 in common.

The rst target current circuit may be traced from junction point 255 through conductors 251, 260 and 26|, center tap |02, the lower half of primary winding l I, conductor 262, target plate 44, the electron beam 31, cathode 32, and conductors 254, 263 and 264 to junction point 256,. A second target current circuit may be traced from junction point 255 through conductors 251, 260 and 26|, center tap |52, the upper half of primary Winding l, conductor 265, target plate 45, electron beam 31, cathode 32, and conductors 254, 263 and 264 to junction point 256. It will be seen that the currents in primary winding |0| due to impingement of target plates 44 and 45 by the beam act to induce opposite fluxes in the core of transformer |3, so that when the beam impinges equally on plates 44 and 4 5 no resultant ux remains to induce a voltage in v secondary Winding |50.

A third target current vcircuit may be traced from junction point 255 through -conductors 251, 260 and 265, center .tap |35, the upper half ,of winding |64, conductor 261, target plate 45, .electron beam 31, cathode 32 and -conductors254, 263 and 254 to junction point 2,553. A'ourth target current circuit can be traced iromjuncticn point 255 through Vconductors 251, 526.2 and 255, center tap |55, the lower half or winding |134, conductor 2,12, target plate (il, ,electron Ybeam `31, cathode 22, and conductors v254, 26.3 and 25,4 to junction point 256. Again no induced voltage appears lin secondary winding .|23 when target plates 43 and 41 are Iequally impinged by the beam.

Since the anodecurrent in even a very eicient cathode ray tube is at most only a few hundred microamperes, and since normally only nearly mutually neutralizing portions of lthis total ow in the transformer primary windings, it is Aobvious that amplification of the -signal must be provided. It has been considered desirable vto make use of a property of the cathode ray ytube to obviate the need of highly sensitive 11C. amplifiers, which are technically dimcult to construct. The property referred to is that of modulation of the beam in intensity, by the applica,- tion of suitable modulating voltage between the cathode and the modulating electrode, so that the target currents have alternating components which are .capable vof separation :fromtheiuniv`directional lcornpcnents and of amplification in a conventional ampliner. For this purpose an alternating potential is impressed between cathode 32 and grid 33, but in order that the grid may not go positive during either half cycle of the alternating voltage, it is necessary that the latter be combined with a unidirectional voltage of a polarity to make the grid at least slightly negative at all times. The grid circuit accomplishing this modulation includes an alternating voltage induced in secondary winding 1c of transformer 65 and the unidirectional voltage drop between slider 8G of potential divider 16 and junction point 256, and may be traced from grid 33 through conductors 21| and 212, secondary winding 1E), conductors 213 and 214, slider 3U, the portion of winding 14 above slider 82, junction point 255, and conductors 264, 253 and 254 to cathode v33.

Condenser 35 is connected between conductors 254 and 21| to reduce the eiect of harmonic or other higher frequency components of the modulating alternating voltage: its impedance is se.- lected to be high to the signal frequency but low to its harmonics, which are thus shunted and do not signicantly affect the bias voltage on the grid.

Since all electrons have the same charge, and hence repel one another, there is a tendency for the beam to scatter and become diffused. This tendency may be overcome by giving the electrons so great an axial velocity that only negligible radial movement due to mutual repulsion can take place in the brief interval during which they are passing between the cathode and the target plates. It is also desirable that the cross sec,- tional area of the beam be as nearly circular as is possible, for reasons discussed in connection with Figures 3 and 4. Accordingly electrodes 34, 35 and 36 are given'positive charges of magnitudes most suitable for the dimensions of the tube. It has been found that electrodes 34 and 36 should be at the same potential as the target plates, this being particularly desirable as concerns electrode 35, because thereby the average acceleration undergone by an electron in moving between electrode 33 and the target plates is zero. The voltage between electrode 3,5 and the cathode may be considerably less, and since the shape of the apertures has a controlling effect kon the area of lthe beam,

they should be accurately circular.

To obtain the voltage relations just described electrode 34 is connected to junction point 255 through conductors 215, 216 and 251, electrode 36 isconnected to junction point 25'5 through conductors 211, 21E and 251, and electrode 35 is connected to slider 1'1 of voltage divider 13 through conductor 285. Slider 11 is adjusted to give a beamdameter of about 3A; of an inch at the target plate.

.Condenser 86 is connected between slider 11 and conductor 253 to reduce the effect of tran.- sient variations in the power supply on the cross sectional area of the beam. A As pointed out above, means must be provided to bring the beam initially to the central posi# tion. For this purpose itis caused t0 pass between the pairs of deflecting plates. If the plates of a Apair are at the same positive potential, they attract the beam equally and have only a slight defocusing veect: if they are not of the same potential the one which is more positive attracts the beam more than vthe kother and lthe beam is ,deectedtoward the more positive plate.

vDeiiecting plate 421s .connected to slider |31 by conductor 2M, and derlecting plate 4| is connected to conductor 252. The left end, of winding @il and the right end oi winding 34 are connected to positive terminal 03 by conductor 283, and are thus more positive than junction point 355. The right end of winding S6 and the left end or" winding 34 are connected to junction point 234 by conductor 235, and are thus less positive than junction point 255. When the sliders are at the centers of their windings deflecting plates l0 and 4i are both at the polarity of junction point 255, and neither has any deilecting eiiect upon the beam. As the sliders are moved to the left, plate 43 becomes more positive and plate 4| less positive, and the beam is deilected in a direction parallel to axis 50, toward target plate d4 and away from target plate 45: if the sliders are displaced to the right the deiiection of the beam is in the opposite direction.

Deflecting plate 42 is connected to slider 3| by conductor 205, and delecting plate 43 is connected to slider 33 by conductor 261. The left end oi winding 02 and the right end of winding 90 are connected to positive terminals 63 by conductor 233, and are thus more positive than junction point 355. The right end or winding 92 and the left end of winding 90 are connected to junction point 204 by conductor 285, and are thus less positive than junction point 255. When the sliders are at the centers of their windings, deiiecting plates 42 and 43 are both at the potential of junction point 255, and the beam is not delected. As the sliders are moved to the left, plate 43 becomes more positive and plate 42 less positive, and the beam is deected in a direction in l parallel to axis 5|, toward target plate 41 and away trom target plate 43: ii the sliders are dis placed to the leit, the deflection of the beam is in the opposite direction.

The sliders are adjusted during the setting up of the system so that with the tube vertical and axis 50 in the magnetic meridian, north being in the direction of the heading of the craft 50, the beam impinges on target plates 44 and 45 equally, and on target plate 41 more than on target plate 46, the center of the spot being deflected toward plate 41 by about l/8 of an inch.

The conditions just set forth result in equal and opposite target currents in the halves of primary winding of transformer i3, and accordingly no voltage from the secondary winding |00 is impressed by conductors 292 and 263 on electronic unit l5, and no output voltage appears between terminals H0 and ||1 of the unit. The target current downward in primary winding |04 of transformer |2 is greater than that flowing upward, and a voltage is induced in secondary winding |03 of the transformer and impressed by conductors 230 and 29| on the input of electronic unit i4. This voltage alternates at the frequency oi the source, by reason of the intensity modulation of the beam: the unidirectional component of the target current is not transmitted through the transformer.

Power terminals ||2 and ||3 of electronic unit I4, and power terminals |20 and |2| of electronic unit |5 are energized from terminals 6| and 62 through conductors 294 and 295. The unit i4 amplifies the input voltage without materially shifting its phase, and rectifies the ampliiied voltage by transmitting only the first or the second half cycles according as the input voltage is in phase (current in the upper half of winding |04 greater) or out of phase (current in the lower half of winding |04 greater) with that at terminals 6| and 62. There appears at output terminals ||0 and for the case when the craft is heading in the direction of magnetic north, a unidirectional, pulsating voltage of such a polarity that the terminal l0 is positive: this cosine voltage is impressed across resistors |24 and |25 by conductors 296 and 231. The common junction point |26 of resistors |24 and |25 is grounded by conductors 30| and 302 and ground connection |83. Condensers |21 and |30, connected between junction point |25 and conductors 236 and 291 respectively, and condenser |3|, connected between conductors 296 and 291, are effective to iilter out the alternating come ponents of the cosine voltage so that the voltage between conductors 236 and 291 is essentially a pure unidirectional voltage which varies as the beam moves between target plates 46 and 41.

The cosine voltage is impressed upon recentering coil I6 by conductors 303 and 304 in such a polarity as to create a magnetic iiuX in the direction of the heading of the craft. This deflects the beam cross-wise of the craft, from plate 41 toward plate 46, and accordingly reduces the signal to electronic unit i4 and therefore the output from the unit. The gain in amplier I4 and the number oi" turns in coil I6 are so chosen that when a condition of equilibrium between the earths Jlield and that of coil I6 is reached, the beam is displaced from its central position toward target plate 41 by about 1/80 of an inch.

Output terminals ||6 and ||1 of electronic unit i5 are connected across resistors |32 and |33 by conductors 305 and 306. The common junction point 301 of resistors |32 and |33 is grounded through conductors 3 0 and 302 and ground connection |83. Filtering condensers |35 and |36 are connected between conductors 306 and 305, respectively and junction point 301, and condenser |31 is connected between conductors 305 and 306 in a structure in every way similar to that described above, to give essentially pure unidirectional sine voltage between conductors 306 and 305: in the condition of the system described above, the sine voltage is zero, corresponding to an angle 0 of zero degrees. Recentering coil is connected across resistors |32 and |33 by conductor 3l'| and conductors 305 and 3|2: since there is no sine voltage no current can iiow in the recentering coil and the beam is unaffected.

The cosine voltage is impressed on ratio meter 20 by conductors 3 3 and 3| 4, and the sine voltage is impressed on ratio meter 20 by conductors 3| i and 3|5 and conductors 305, 3|2 and 3|6, and the needle of the meter takes the position correspending to the tangent of 0; 0 in this case equals Zero. 1f it is desired to compare the heading of the craft at any time with the magnetic north, the zero of the ratio meter is brought to alignment with the needle at this point.

Resolver 23 is set by manual adjustment of shaft |5| so that its angle qb is as nearly zero as possible. The cosine voltage is applied to terminals |43 and |44 of resolver 23 by conductors 303 and 3|1 and conductors 304 and 320. The sine voltage is applied to terminals |45 and |46 of the resolver by conductors 306 and 32| and conductors 305 and 322. If the setting to zero of the angle of resolver 23 has been exact, no Voltage appears at output terminals |41 and |50 of the resolver (as will be indicated by lack of operation of motor 200). If the setting is .incorrect, terminals |41 and |50 are not at the samepotentialf, andf tht-samelvoltagetfdifterence is conducted toi-liked contacts |12 'and' .|f1--3ioffinf'f terrupter-21 by conductors 323 and 324.

Movable contact |.1?| of interrupter. 21 is connected to ground through blocking condenser |83-, winding |84:`of.A potential: divider |85, conductor 325` andyground. connection; |83; Etuis maintained inmotionatl the frequency of`A the A. 'C. supply: by: voltage yl'ecl from: terminals. 6i and .62` byl conductors3 Maand 33|Land conductors 321 andy 33|. to! the. primary: |13 of transformer |15, and: from. the secondaryk |14 `otthe trans formerbyxconductor 332, ,phasing condenser 329 and conductor.- 333lto. windingy |1181 of. the interu rupter. A portion off.' ther fundamental.. alternating component or the square ware voltage resulting on. movable; contacts'v |1.'|A is. impressed on the input of amplifier 5r by: slider 83; and conductor` 338.` Thevamplifier is::also. supplied with alternating voltagelfrom. the source byconductors. 32|1and13341` andconductors 321;.and: 335".

4If the input voltage andtt'he.powervolta-ge are ofi the same` phase, motorI 230! is. energized through conductors-333'; 331;l andr 346; toA oper-ate in a4 forward. direction.- and ifv the; input voltage isof the. opposite phase theimotor is energized to opt-irateiin.v the revcnse: direction. Operation ofrthemotorisan indication thatresolver. 2.? is not-correctly adjusted, and-shaft v|51 is manually rotateduntil': the. operation of motor 233 stops; The resolver is now set-"accurately to an angle qs of zero: indexabmay-be setto indicate north on scale 203 andzmotor-200emay becoupled to shafts |5| and 20|.

Resolver`4 2liis setV by manual adjustment oi shaft 2|2 sothat-angle 4 isfas'nearly zero as possible; vThe cosinevoltage is applied to terminals204 and v23510?resolver24 by conductors 303, 3|1and-34L andlfconductors 304, 320 `and 342; The sine voltagezisrapplied to terminals 206, 201 of the resolver by conductors 32| and Maand conductors 322' and 31W- If-fthe'setting-to zero of the angle qa of-'1esol-ver-24'fhas been-exact, no -voltage will appear atoutput terminals 2H) and 2|| of the resolver aswill be indicated byL lack of energization of torque-motor232-i Ifithe setting is incorrect, terminals-21| 0- and` 2 |-are^notf at the samepotential, and the Lvoltage difference is -conducted to xed contacts 2| 3 and 214 of vinterrupter 23 by c onductprs345fand 3462 Movable contact 2|??I of interrupter 28 is connected tQ; groilncl through blocking condenser 2H; winding 22|) of potential di-` vider 22|, conductor-341 andjground connection |38. 1t is-maintained in-motion at the-frequency ofthe A. G. supplybyvoltageY ledf from terminals 5| and G2 throughrconductors-326 and 3 30 and conductors- 32-1` and- 33| to ther primary |16 of transformer andfromthe secondary/|145 of thetransformer by'conductors 332 and 333` and phasing capacitor'349ito-winding2|6. A' portion ofV the fundamental alternatingi component of the` square wave vol-tage resulting on movable contact 2| 5 isimpressed onf the inputl ofampliiier 26 by slider 222 and `conductor-35H; The amplifier 2 is also supplied;lr with alternating voltage from the source -byvconductors 326' and35-2 and conductors. 3221** and- 3 51| if the input' voltage and' the power voltage are of the same phase; torque motor'23-2 is energized: through conductors `353,-- 3-54: and 355` toV operate. inav foi-ward direction, and if theinput voltage-is of.- the oppositelphase-:the motor is energized: to.A operate; 'ini ther reversedirection.

Operation: of :themotonV 'is' anfindication -that1reaccuses" IS solver 21k-is not correctly adjusted, andf shaftv 2`I2 is manuallyr rotated until operationv off motor 232 stops. The resolver isv now set accurately to an angle of'zero: .gyroscope 22 may be coupled toshaftZ'l 2 and` energized, and index 24| may be set toindicate north on scale 240;

'Operation Having been set up and.. adjusted as indicated above, the operation of the system is as follows. So lionel as, the heading of the craft lies in the magnetic meridian, no change inthe direction of the beam. withv respect to the target plates takes. place Accordingly there is no change. in the sine and. cosine voltages, the indication of ratio meter remains unaltered, and motor 2,00 remains unenergized so that the indication of indicator 2| does. not change. Torque motor 232 also remains unenergized` as long as the gyroscope-does not drift with respect to thezcraft: it

- will be realizedV thatso long as. theheading of the craft, remains the same, any movement of the gyroscope with respect. theretois due to drift of the-gyroscope, andresults'in rotation of shaft 2| 2 ofresolver 211.v When such rotationtakes place, angle qb, is no longer equalY to angle @and fixed contacts 2|3 and2|4 assumedierent potentials with respect to ground. This results in theappearancepof an'` alternating voltage on the input of phase sensitive amplier 23, which resuits. in energization of torquemotor 232 in such a sense as to-precess gyroscope 22 back into its original alignment. Thisl actuates shaft 2`|2 to adjust angle c until it is again equal to angle 0, whenenergization of the torque motor ceases.

lf the heading of 'the craft changes, two effects occur simultaneously. The rst of these eiects is a change in the position of the beamfwith respect to the target plates: the second eiect is a movement-of the resistance members of'resolver 2li'with'respect to the gyro stabilized shaft 2|2. The sine. and cosine voltages are nowv functions ostiay new angle.v 0- and ratio meter 20 indicates this. new angle.` The angular position of the sliders of resolver 2li has a new value qb'. Since both thef-compassand the resolver are mounted in thevcraft andl move unitarily through the same angle, is equal toc', and if the torque motor system was-inbalance-before the heading of the craft changed, it will remain inbalance through-l out the change `in heading.

So far as the relationship between the compass andthe directional gyroscope is concerned, it maybe briefly expressed as follows. The two instruments are mounted for unitary azimuth displacement, and the compass has-no tendency to permanent drift away from the magnetic meridian,v while the gyroscope does have a tend'-v ency toY drift away fronrits original heading. After theinstrurnents are brought intooriginal coordination, no sustained signalfrom thecompassv is appliedto the torque motor of the gyroscope so-long as the two instruments remain in the coordinated relationship. The only thing which can disturb this coordinated relationshipv is drift of thegyroscope from its originalposition, andwhen this takes place its new relationship'withrespect to the compass resultsfina resolver output motor-to bring the nated relationship. -v If desired-theoutput,ofiV amplifier 23 may be applieddirectly to arudder servomotor instead ofbeing usedI to precess thedirectional gyroscopa-buty thisis not/the preferred modeof practicingtheinventiom M 1 gyroscope back into coordivoltage which energizes torque Turning of the craft does not cause any relative movement between the windings of resolver 23 and its sliders, so fixed contacts |12 and |13 assume different potentials with respect to ground. This results in the appearance of an alternating voltage in the input of amplifier 25, which results in energization of motor 200 in such a sense as to move the sliders toward a new position in which angle p' is equal to angle 0. When this condition has been reached, the motor is deenergized, and index 202 has been driven to a new position with respect to scale 203 which indicates the new heading of the craft.

In the embodiment of the invention shown in Figure 1, the following values of components were found satisfactory.

Resistors 8 microfarads. .25 microfarad. 1.25 microfarads.

Voltage of secondary 67 6.3 volts.

Voltage of secondary 70 25 volts.

Voltage between 63 and (i4 -100 v. D. C.

Voltage between 61 and 62 115 v. 400 cycles 1 phase A.

Structure of the modification of the invention Figure 2 illustrates a simplified modification of the invention in which many of the components, particularly those relating to the recentering of the beam, have been omitted, together with their functions. For purposes of illustration the showing of the ratio meter and the motor indicator has not been repeated in this figure, the directional gyroscope only being shown. l

The system of Figure 2 comprises a cathode ray tube 4|0, a power supply 4|| for the tube, a pair of transformers 4|2 and 4|3 coupling the output of the tube to a resolver 4 |4, and a transformer 4| 5, coupling the resolver to a phase sensitive amplifier 4|6, which energizes the torque motor of directional gyroscope 4|1.

Cathode ray tube 4|0 is shown to comprise the usual envelope 420 Yenclosing an electron gun comprising a heater filament 42|, a cathode 422, a control electrode 423 referred to as a grid because of its function rather than because of its structure, and a plurality of focusing and accelerating electrodes 424, 425, 426 and 421. The tube also includes a plurality of defiecting plates 430, 43|, 432 and 433 and a plurality of target plates 434, 435, 436 and 431, and is coated on its inner surface with a conducting layer 440. The tube is pendulously mounted in an inner support ring 44| connected by diametrically opposite pivot pins 442 with an external ring 443: the latter ring is mounted, on diametrical pivot pins extending at right angles to pins 442, in any suitable support member, not shown. It is to be noted that in tube 4|0, the electron beam proceeeds downwardly, while in tube the beam proceeded upwardly. It is also to be noted that in connection with tube 4|0 there are no recentering coils.

Power supply 4| is shown to comprise a transformer 444 having a primary Winding 445 and a pair of secondary windings 446 and 441. The transformer is designed for energization with an alternating voltage applied to input terminals 6| and 62. A second pair of input terminals 452 and 453 is arranged for energization from any suitable source of unidirectional voltage, the polarity being such that terminal 453 is positive and terminal 452 is negative. Power supply 4|| also includes fixed resistors 454 and 455 and the windings 451 and 460 of a pair of voltage di# l viders 46| and 462 having sliders 463 and 464 respectively. i

In a copending application, Serial No. 771,265, filed August 29, 1947, now Patent No. 2,505,261, granted April 25, 1950, in the name of Richard Syrdal, and assigned to the assignee of the present application, there is a complete disclosure of details of the structure of the cathode ray tube indicated at 4|0 in Figure 2. For details of the structure, energization, and function of this tube per se, reference is made to that application.

Transformer 4|2 comprises a primary winding 654, having center tap 655, and a secondary winding 656. Similarly, transformer 4|3 comprises a primary winding 651, having a center tap 660, and a secondary winding 66|. If an A. C. ratio meter or differential voltmeter were to be used with this modification of the invention, it would be connected to secondary windings 656 and 66|.

Although the resolver shown in Figure 6 functions satisfactorily in the modification of the invention shown in Figure 2, I prefer to use a modified resolver shown in detail in Figure 7. The modified resolver is shown to comprise a pair of resistance units 662 and 663 comprising respectively resistance members 664 and 665 and sliding contacts 666 and 661 operated by a common shaft 410. As best shown in Figure 7, resistance member 634 comprises a substantially fiat form 41| around which there is a winding 412 having a center tap 413. Similarly resistance member 665 comprises a winding 414 with a center tap 415 wound on a form 416 of insulating material. Windings 412 and 414 are of extremely fine wire, and are put on the forms with a uniform advance. If desired all forms may be slightly convex to aid in maintaining the windings tight and uniform.

Electrical connection is made to the ends of winding 412 by conductors 411 and 480, and to the ends of windings 414 by conductors 48| and 482. Sliders 666 and 661 are mutually insulated, and electrical connection is made thereto by conductors 483 and 484, respectively. Center taps 413 and 415 are electrically interconnected by conductor 485.

Transformer 4|5 is shown in Figure 2 to comprise a primary winding 486 and a secondary winding 481, and functions to couple conductors 403 and 484 of resolver 4|4 to the input terminals 490 and 49| of amplifier 4|6.

Amplifier 4 I6 further comprises a pair of power terminals 492 and 403, and output terminals 494, 495 and 496. The amplifier is of the same nature as amplifiers 25 and 26 of Figure 1, and its output energizes the torque motor of directional gyro.. scope 4|1, which also is of the same nature as that of directional gyroscope 22 of Figure 1: the torque motor of directional gyroscope 4|1 is not specifically shown, but it will be realized that an arrangement such as was previously described is included in gyroscope 4 1.

The gyroscope is arranged for connection to shaft 410 of resolver 4|4 so that the position of sliders 666 and 661 is controlled thereby. The gyroscope also stabilizes another shaft 491 which may be unitary with or distinct from shaft 410, and which actuates a slider 500 with respect to a winding 50| to comprise a voltage divider 502 forming for example a part of the automatic pilot of the craft to which the compass system is mounted. Winding 50| is mounted for pivotal 2f movementabout theaxis of shaft 431'; the mount beingprovided with-adjustingmeansvr such as'gear teeth 503" engaging a. pinion 504 actuated by a manual knob 535.` The mount also carries an index 5t5-for adjustment with-respect to a fixed scale of azimuth 501.

Circuit co11.11.ectz'ons` of the modjcatz'on Since muchV of the explanatory. matter given inV describing the connections between power supply, 1i and. cathode ray tubev 150i.. Figure 1` ap.- pli'es equally well. to the. connections between power supply 41.1 andcathode ray 4.1.6, this matter Will not be repeated. Primary winding 445 of transformer 444 is energized. from terminals 61. and 52 through conductors 5.14. and 511. Heater iilainentv 421 ofthe cathoderay tube is energized from secondary Winding 4550i. transformer 4.44 through conductors 512, 513 and 514, and cathode 422 is connected to one side of heater lament 421 by conductors 513, 515A and 5118. A voltage alternating about a central'negative value is applied between cathode 422 and grid 4.23 of cathode ray tube 41B ,through a circuit which in.- clud'esV conductors 514, 515 and 516, junction point 5111 resistor 45.14, junction `point 520, secondary winding 44.1 and conductor 521., in such fashion that grid 423'never becomespositive with respect to cathode 422. A suitable unidirectional voltage drop is maintained in resistor 454 by connection of the resistor in a series circuit which may be traced from terminal 453' through conductor 522, junction point 523; windingAil, june tion point 524', winding 45.1', junction point 525, resistor 455, junction point 511, resistor 454junction point 520, and conductor 521 to terminal 452. From thisit will be seen that junction point 520 i's negative with respectv to junction point 511, with' respectto which' all' thelother junctionpoints are positive.

Electrodes 424 and `421i are. maintained at the highest positive potential, that of junctionv point 523, by means of conductors 530, 531 and' 532. Electrode 42545 maintained atV a much less positive potential with respect to cathode 422` by a conducto;l 533 which connects it with junction point 525; Electrode 421' is maintained at apotential slightly less than maximum positive potential by a conductor534'whi'chA connects it with junction pointA 524'. Delecting plates 430 and 432 and conductingv layer 440v are maintained at the same potentialk as vanode' 421"'byconnection theretointernal ofthe-tubeindi'cated' by reference numerals 535, 535, 531l and 533.V The potential of deecting plate 431 is maintained adjustably equal to or greater thanthat oi deflectingplate 4351 by a conductor 54'0- which connects it to the slider 454 of Voltage divider 452. The potential of deiiecting plate 433 is-maintained equal to or less than the potential of deilecting plate 432 by an electrical conductor-541 which connects it to slider 45S ofV voltage dividerV 451. It will Vbe understood that in the construction ofthe tube the electrodes are so arranged that' if' there is any tendency for the beam to be off cen-teh; this will take place inl the direction of plates 433 and 43m-so that the adjustment available by sliders 453 and 454 will be -theproper sense to center thelbeam.

As in the tube of Figure 1 four target current circuits may betraced. The rst of these circuits may be traced fromv posi-tive junction point 523A through conductors 542 and1'54'3, center tap 555, the upper portion ofwinding 654-, conductor 5441,.target plate 434, the elec-tron beam 4191, cathode 422,'conductors-518 andf516; junction point: 5511,` and resistor 454, to negative junction point 520. The second circuit followsthe same path, except that. between center tap, 5.55: and electron beam l1-Sit traverses the lower portion of windingV 554,' conductor5f45: and target plate 435. The opposition of `target currents and there,- fore of induced fluxesy in the `,core of: transformer 412 is obviously the same as that discussedy in FigurelO;

Similarly, a third target, current circuit may be traced from positive junction pointI 523 through conductors 542 .and 545; center tap 550, the upper kportion ci'v winding 551,. conductor 541, target plate 431, elect-ron beam 4.19; cathode 422, con.- ductors 553 and 5113, junction point511, andresistor 45d to negative junctionpoint 523; The fourth` targetV current circuit follows the same path, except betweencenter tap 550 and electron beam 413'it traverses the lower portion .of winding 55?, conductor 55iland target plate 436; Here again the opposition ofr target currents-and resultant fluxes in transformer 4.13 is the same as that described in Figure l.

Input conductors 4:11 and 430er resolver 41.4 are connected to secondary/winding 6560i transformer 41.2, and input conductors 481 and 482 of resolver 41,4 are connectedtosecondary Winding 35i of transformer 41.3, respectively. Output conductors 433: and .43d of resolver 4.1.4.. are .connected to primary lfof transformer 4.15, and secondary winding 431 is.v connected tov input terminals 495 and 431 of amplifier 416 by conductors 551 and 558. Powerterminals 492 and 453 of amplier 415 are energized from terminals 51 and 52 through.v conductors-552 and 5,53, and the torquemotor of directional gyro. 41,1 is .ener-f gized from terminals 494, 495 and. 4350i amplifier 415 through conductors 556, 555, and 554. Conductors 551, 550. and 55,1L lead from voltage divider 502 tothe automatic pilot circuit.

In setting up the modied system, tube 415 is mounted in the aircraft so that the line of action of deliecting plates, iljlva-nd4 431-l is across, and that of plates 432 and 433 is along the longitudinal axes of the craft, which is oriented so that its heading is in the magneticmeridian. Shaft 491 is disconnected .from gyroscope 411,. slider 5133 is set at the center ot Winding 5.01, index 5.55 is set at north on scale 501, andv the azimuth function of the automatic pilot is. set for straight flight.

SinceA the electron` beam is directed downwardly instead.- of upwardly, the earths magnetic field this time deilects it to the leftin the gure rather than to the right, that is, tothe west rather than tothe east, so that target plates 43,6 and 431-are equally iinpinged while target plate 434 isinipinged toa greater extent than target plate 435. Equal and opposite primary currents, flow in*V transformer 4123 accordingly no output voltagel appearsacrosssecondary winding 35-1- of the transformer. On the other hand the target current in the upper'fportion of primary winding of transformer-4t2 exceeds that in the lower portion of; the lwind-ing, and an output voltage appears insecondary Winding 655 and is im pressed' upon the windingy 534- of resistance unit 632. One of the differences between the modication of Figure 21and the modication of FigE ure 1 is now quite evident, in `that the voltages on the resolver resistance members in Figure 2 are of alternating character, While those in Figure 1 were of unidirectional character. The amplitude of the output voltage of transformer 412 is nevertheless` proportional to, the. cosine of.. the

angle 0, and that of transformer 4|3 is proportional to the sine of angle 0.

Referring now to Figure '7, it will be apparent that any rotation of shaft 41|) causes movement of slider 66S with respect to winding 664. The component of this movement perpendicular to the direction of the wires of the winding causes a marked change in the resistance between the slider and center tap 413, since it includes more and more turns of the resistance wire. Contrariwise, the component of the movement of slider S66 parallel to the direction of the wire has little effect on the resistance between sliders B66 and tap 413, which at most can be changed in resistance only by that of less than half a. turn of the wire as compared with a maximum resistance change equal to several hundred turns in the other direction. It may therefore be said with sufficient accuracy for the purpose of the present invention that the resistance between L slider 656 and center tap 413 varies with a first component of the movement of the slider, which in turn is proportional to the sine of angle In the same manner the resistance between center tap 415 and slider 661 is proportional to a second component of the movement of the slider at right angles to the first component, that is, the sine of (90{) or to the cosine of q'.

The applied voltage between conductors 411 and 480 is proportional to cosine and the voltage between the center tap 413 and slider 666 is therefore 0; 0 (sin s) The applied voltage between conductors 48| and 482 is proportional to sine 0, and the voltage between center tap 415 and slider 661 is therefore as s The voltage difference between sliders 666 and 661 is o 2 (Sm d0* When e equals 0, the two terms are equal and 4 the voltage difference becomes zero: resolver 4|4 accordingly functions in a fashion similar to re solvers 23 and 24 in Figure 1 to give an output voltage which is zero when angle e of the resolver is equal to the angle 0 of beam deflection: the output voltage is alternating and reverses in phase as rp is greater or less than 9, just as the unidirectional voltage output of the resolver in Figure 1 reverses in polarity according as p is greater or less than 0.

Amplifier 4I6 in Figure 2 functions to energize output terminals 494, 495 and 496 in a first or a second fashion, according as the voltage supplied by transformer 4|5 is in phase or out of phase with the voltage supplied to power terminals 492 and 493, and the torque motor of directional gyroscope 4|1 is energized in a forward and a reverse direction accordingly, precessing the gyroscope to adjust angle p by operation of shaft 410, and to control the automatic pilot by rotation of slider 500 with respect to winding 50|.

In the original installation of the system angle p is set as close to zero as can be. As before, operation of the torque motor of the gyroscope is an indication that the setting is not exact, and it is adjusted until operation of the torque motor stops, after which shaft 491 may be coupled to the gyroscope.

Y Operation The operation of the modification of the 1nvention is the same as that of the modification previously described. As long as the gyroscope does not drift in azimuth, no signal voltage is transmitted to the torque motor: change in the heading of the craft changes angle rp and angle 6 by the same amount, and no energization of the torque motor results. If the gyroscope does drift, sliders 466 and 461 are moved, angle `qi is no longer equal to angle 0, and a voltage is supplied to amplifier 4|6 of such a phase as to cause energization of the torque motor in a sense to precess the gyroscope back into alignment with the magnetic meridian, and to correct any erroneous signal being supplied to the automatic pilot due to voltage stabilization of slider 503.

It will be evident that each of resistance units |53, |54, 662, and 663 functions in the apparatus as though it were an anisotropic resistance element, that is, an element whose resistivity is not the same in all directions.

In the foregoing specification there are disclosed improved means for preventing the loss of azimuth in a directional gyroscope by slaving it in a novel fashion to a cathode ray cornpass, as well as means for obtaining a remote indication of magnetic heading from such a compass. The means are shown to comprise a novel angle repeating system and also to comprise means for minimizing the effects on the controlled unit of defects in the eld sensing unit. As a subordinate inventive contribution there are disclosed details of two particular variable resistance units, and the application of the system to the control of the craft in azimuth is also clearly described.

It should be pointed out that the field sensing system disclosed herein is not limited to compass applications, but may be used wherever indication or control in response to a magnetic eld is desired: geophysical prospecting is an example of another eld to which the invention is applicable.

Numerous objects and advantages of my invention have been set forth in the foregoing description, together with details of the structure and function of the invention, and the novel features thereof have been clearly described. The disclosure, however, is illustrative only, and I may make changes in detail, especially in matters of shape, size and arrangement of parts, within the principle of the invention, to the full extent indicated by the broad general meaning of the terms in which the appended claims are expressed.

I claim as my invention:

l. A compass system comprising in combination: a cathode ray tube having an electron gun, emitting a, vertical beam of electrons deiiectable by a magnetic field, and sector shaped target plates mounted in symmetrical pairs for variable relative impingement by said beam to give variable target currents; means connected to each pair of oppositely disposed plates to derive from the difference between the target currents therethrough a voltage determined thereby, voltages being proportional to the components of said magnetic field along the pair of axes about which said pairs of plates are respectively symmetrical; a `resolver comprising a pair of voltage dividers, each including a resistance unit and a slider making movable contact therewith, and means mounting said units and said sliders for simultaneous relative movement so that the output from each voltage divider is a function of said movement; means impressing said vo1tsaid connected to salia sliders rerg saiomove- 'men-t; voltage respbnsive means ener'g ng said motor lmea-nswhen*said slidersar'e net at the same potential; actuatedrby operation oi "said motor.

2. -In-rcornbination: eath'o'deray tube having an electron gun, 'directing a gan vaxis 'a de- Aiectable beam 'of electrons dulafted `lintensity, and yquadrantal target plates lmounted about said axis in opposedpairs symmetrical :about horizontal axes lfor variablel -impingement by 'said beam to give 'variable' target cuirents; means pendulously mounting said tube for de- `iection `of said beam 'by the earths magnetic nem; means connectedto 'caen-pair of said plates for deriving from the difference bettv'eeii'the target currents thereof :an alternating voltage determined in phase and 'amplitude bysaid 'diiference; an amplifier kand phase'sensitive rectiilerv deriving iliona reach said alternating' voltage a unidirectional voltage the `tilde Aof which are determined :bythephase and ,amplitude of said alternating voltage; a controllen member actuated in accordance with said unidirectional voitages; I,means for electrically deilecting :said :beam in the direction of each said horizontal axis; and means applying said unidirectional voltages to' :said last'named means in agdegenerative `feedback .system to almost completely opposefdelectionvoffsaid beam by the earths magnetic field, `thus limit-'ing the actual movement of, the beam Land hence minimizing inaccuracies in the actuation of the controlled member due to nen-,circularity of said beam and non-emialityof said ampliers .and ci said yrect# AGIS. t

i 3x. In combination: f. a rrst resistance unit; means applying across aidtunit -a rst `,voltage proportional to the -cosineuof a selected iangle; a first slider rotatablegwith respect tolsaid first unit so that the potential `of said slidei'vvith respect `to a reference vpoint `varieswith a rst component of tite mov-.ement of said :slider andis relatively unaifectedby a seeondr'component of said movement; a second resistance unit; means V:al'plying across said unit a second voltage proportional to the sineof saidselected angle.; a 'secfnd slider ro'- tatablewith respect to said second unit :so .that tne potential of slider with respect 'to .said reference Apointpis `-relatively unaitec't'ed by a 'rst ccmpcnentof the movementpoi:said-second.slider an@ varies witna second :component 4of saidmovenient; means mounting said run-its .so .that said .nrstccmponentshave theisamedirectiongand said second-components are directed perpendicular thereto; and means causing :simultaneous mov 'ment @isa-id sliders-trom a normal :position in passingnthrougn AWhiclirsaid plirstslider is sub# vject to maximum rate ofchange of potential and second slider .is .-subj ect to ,'ininimu-m Vrate 'of 'se of potential, ,whereby:saidsliders assume the samegpotent'ial when rotated -zrom 'said inormal position by said selectedanglef. f i

4. In combination; :a pair jof, resistance units cachot which comprises apair of rectilinear ires' fee members 'cfpedual length, means insulat.. gly 4mounting 'said :members `:to form 'the Joplpcsite sides of ra square, a pair oi electrically conducting Vimentdners completing said sanare *and each `connected. to vone 'end of *each *of said lire- ,'sistence mem-bers', 'and a "single slider :pivoted IVat the center of said vfsquar fior electrical connection wit saidaneinbersatxanysin'glespot along tbeiperipliery b'fssadsqrarermeansfmunt;

and heading indicating means polarity and magniv a :resolver comprising a `iisgV said units so that the resistance members of tion from a normal posit-ion in vr is at the center of one of 'said re stante bers and the otherl slider Cis 'at the center of Vone of said consuming members; mea-ns ma" fg electribal connect-,ieri 'to' "said contracting mesi-19ers arid said sliders; and means for causing rotation of said slider. g

5. In combination; a pair of resistance lu ts each of which comprises a resistance vvin ing having at least one substantially plane surface f rectangular `nl utlirie, a :slider pivotedfabout Van anis substantially perpendicular to' the echter of said surface, and-making contact therewith along Ya circie Whose diameter is not greater t-lian'tli'e shortest dimension `ofA said rectangular surface, so that .at tWo points along said circle said slider vis lmoving perpendicular to Athe v'vires of said Wind'- in'g and vat .points'90 degrees latera'long 'said fc'icle, said slider is moving parallel to the Wires of said Winding; means short ircuiting those of the Wires `of `said Winding extending from said last named points to the adjacent ends fof said winding, and tap means making electrical connection to said'v/inding midway between said last named points; means insulatingly mounting said units-so that said planes aresubstantially parallel; 4means insulatingly connect-ing said slders'ffor. unitary rotation, from a normal position'in Which one of said sliders is at one of said rs't 'named .points and the other slider is at on'eof said last named points; means electrically' connect-ing said tap means; means energizing" said windings with lvoltages Whose magnitudes are sine and cosinel functions of a variable; and voltage responsive means :connected betweensa-id sliders for simultaneously `metrieal lildrsor variable impingement by said .beam toY give variable target currents; means for electricallydenecting said beamindepenfdentlyfof saidflel'd; means connected to each pair of optpositely disposed plates to derive vfrom `thegdiifeia ence between the target currents thereof a volt; :age determi-ned thereby, said rvoltages being proportional to thecomponents of the earths mag- -netic -eld along' thepair 'of axesabout which Esaid pairs of lplatesare respectively symmetrical; pair of resistance units, apair of sliders making movable contact therejvvithand means Vmounting said units and said sliders for simultaneous -relative movement; means impressing said voltages upon said re =sistance iunits, motor ln'iea'ns for causing said `:movement when said sliders are not at the saine potential, and controlled means actuated 'bv 'op'- `eration of said'm'otor and coordinated with the -alignmentof said field Withonef-'o said axes; 'and degenerative 'feedback means, including said .beam deflecting means, whereby said ioltages are effective to reduce tlieactual jdeflection of said `bean-1 'inresponse tosaid field, so as to minimize .the effect on sajdcontrolled member of -nonu'nilformity cfgs'aid "beam andl nonsequivalencein said voltage derivingmeans.

7. fA .compass vsystem comprising, in combina# tion: acatho'd'e raytubet-havngfan intensity mdulated beam of electrons deiiectable by the earths magnetic field and target plates impinged by said beam in accordance with the deflected position thereof, so as to give a pair of alternating voltages varying in amplitude and phase with the magnitude and polarity of the components of the earths magnetic eld along a pair of horizontal mutually perpendicular axes; an amplifier and phase sensitive rectier deriving from each alternating voltage a unidirectional voltage determined in polarity and magnitude by the phase and amplitude of said alternating voltages; means utilizing said voltages to partially return said beam from its deflected position; a resolver comprising a pair of resistance units, a pair of sliders making movable contact therewith, means impressing said voltages upon said resistance units, and means mounting said sliders for simultaneous movement relative to said units, to cause a unidirectional voltage to appear between said sliders; means converting said unidirectional voltage to alternating voltage of a phase and amplitude determined by the polarity and magnitude of said unidirectional voltages; motor means for reversibly causing said movement of said sliders in accordance with the phase of said last named alternating voltage, to move said sliders to a position in which they are at the same potential; and controlled means actuated by said motor means.

8. A device of the class described comprising, in combination, a reversible motor, an electronic ampliiier energizing said motor in accordance with the sense of a signal voltage, electron discharge means including at least three target electrodes through which the discharge thereof takes place to comprise target currents, which vary in interdependent relationship with condition responsive variation in said discharge, and variable means combining the effects of said currents to give a single sense reversing signal voltage, and applying said voltage to said amplifier.

9. In combination: means giving signal voltages proportional to the components of a magnetic field along a pair of horizontal intersecting axes, including means subject to angular displacement in response to said iield; and a resolver, including a member to be controlled in accordance with said angular displacement, a first resistance unit whose resistivity along a iirst axis is negligible in comparison with its resistivity along an axis normal to said iirst axis, means applying one of said signal voltages across said unit, a first slider movably engaging said first unit so that the potential of said slider with respect to a first reference point on said unit varies with the component of the movement of said slider parallel to vsaid second axis and is relatively unaffected by the component of said movement parallel to said first axis, a second resistance unit whose resistivity along a first axis is negligible in comparison with its resistivity along an axis normal to said first axis, means applying the other of said signal voltages across said second unit, a second slider movably engaging said `second.

unit, so that the potential of said second sliderV with respect to a second reference point on said second unit varies ywith the component of the movement of said second slider parallel to said second axis and is relatively unaffected by the component of said movement parallel to said first axis, and means responsive to differences between the potentials of said sliders for causingr movement of said member to be controlled and also causing simultaneous movement of Sad sliders from a normal position in passing through which said first slider is subject to maximum rate of change of potential and said second slider is subject to minimum rate of change of potential.

10. In a device of the class described, in combination: a resistance unit comprising a pair of rectilinear resistance members of equal length; means insulatingly mounting said members to form two opposite sides of a square, a pair of electrically conducting members of effectively zero resistance completing said square and each connected to one end of each of said resistance members, and a single slider pivoted at the center of said square for making electrical connection with said members at any single spot along the periphery of said square.

ll. Apparatus of the class described compris-V ing, in combination: a reversible motor; an electronic amplifier energizing said motor in accordance with the sense of a signal voltage; a rebalanceable motor control system connected to said amplifier, said system including a cathode ray tube having two pairs of target electrodes symmetrically disposed with respect to each other about an axis of said tube and means directing a beam of electrons along said axis for impingement on said electrodes to comprise target currents, means mounting said tube with its axis vertical so that the effect of the earths magnetic eld is to cause the beam to be deflected from'a normally vertical position in which said target currents are equal, means for combining said target currents to produce a single signal voltage whose sense is dependent upon the deflection of said beam from said vertical position, and means for rebalancing said system to reduce said signal voltage to zero; means driven by said motor to position said rebalancing means; and controlling" means driven by operation of said motor.

l2. Apparatus of the class described comprising, in combination: a reversible motor; an electronic amplifier energizing said motor in accordance with the sense of a signal voltage; a rebalanceable motor control system connected to said amplifier, said system including a cathode ray tube having two pairs of target electrodes symmetrically disposed with respect to each other about an axis of said tubegand means directing a beam of electrons along said axis for impingement on said electrodes to comprise target currents, means mounting said tube with its axis vertical so that the effect of the earths magnetic field is to cause the beam to be vdeflected from a normallyf vertical position in which said target currents are equal, potentiometric means for combining said target currents to produce a single signal voltage whose sense is dependent upon the deiiection of said beam from said vertical position, and means for adjusting said potentiometric means to rebalance said system so as to reduce said signal voltage to zero; means connecting said motor in driving relation to said adjusting means; and controlling means driven by operation of said motor.

13. Apparatus of the class described comprising, in combination: a reversible motor; an electronic amplifier energizing saidrmotor in accordance with the sense of a signal voltage; a rebalanceable motor control system connected to said amplifier, said motor control system including a cathode ray tube having two pairs of target electrodes disposed at right angles with-respect to each other and means directing a beam of electrons ,axially 0f said tube for impingement on said electrodes to comprise target currents, means mounting said tube with its axis vertical so that the eiect of the earths magnetic field is to cause the beam to be deflected from a normal vertical position in which said target currents are equal, means for combining said target currents to produce a pair of voltages varying in accordance with the components of the earths magnetic iield along a pair of mutually perpendicular horizontal axes, means combining portions of said voltages to comprise a single signal voltage for said amplier, and means for rebalancing said system to reduce said signal voltage to zero; means driven by said motor to position said rebalancing means; and controlling means driven by operation of said motor.

14. In a telemetering system, a pair of potentiometers each comprising two spaced conducting members, diametrically opposed resistance paths between said members and equal in extent therewith, and a rotatable contact arm to engage said members and said resistance paths respectively throughout successive sectors of its rotary movement, the contact arm associated with each potentiometer being mechanically coupled to the other contact arm and electrically coupled to an indicator, the angular positions of the points of engagement of said contact arms relative to their respective conducting members and resistance paths diiering by a xed predetermined angle, means for establishing a predetermined difference of potential between said members, and means responsive to the variable potential difference between each contact arm and a given reference potential for furnishing a signal according to said variable potential differences.

15. In combination: means subject to unlimited angular displacement from a predetermined orientation; means giving voltage outputs pro portional to the sine and cosine respectively oi the angle of any such displacement; an indicator of angular displacement continuously adjustable from an indication of zero displacement; trigonometrically characterized, endless voltage dividers connected for adjustment concurrently with said indicator so that the ratios of output to input from said voltage dividers are proportional to the cosine and sine respectively of the angular displacement indicated by said indicator; means supplying said voltage outputs to the inputs of said voltage dividers; and means combining the outputs of said dividers to give a control signal which becomes zero when the angular displacement indicated by said indicator is equal to that of said first named means.

16. In combination: means subject to unlimited angular displacement from a predetermined orientation; means giving voltage outputs proportional to the sine and cosine respectively of the angle of any such displacement; an indicator of angular displacement continuously adjustable from an indication of zero displacement; trigonometrically characterized, endless voltage dividers connected for adjustment concurrently with said indicator so that the ratios of output to input from said voltage dividers are proportional to the cosine and sine respectively of the angular displacement indicated byl said indicator; means supplying said voltage outputs to the inputs of said voltage dividers; means combining the outputs of said dividers to give a control signal which becomes zero when the angular displacement indicated by said indicator is equal to that of said rst named means; motor means for adjusting said indicator; and means causing operation of said motor means in accordance with said -control signal, so that said indicator continuously indicates the angular position of said iirst named means.

17. In combination: a pair of resistance units each of which comprises a resistance winding having at least one substantially plane surface of non-circular outline, a slider pivoted about an axis substantially perpendicular to the center of said surface, and making contact therewith along a circle whose diameter is not greater than the shortest dimension of said surface, so that at two points along said circle said slider is moving perpendicular to the wires of said winding and at points later along said circle said slider is moving parallel to the wires of said winding, means short-circuiting those of the wires of said winding extending from said last named points to the adjacent ends of said winding, and tap means making electrical connection to said winding mid-way between said last named points; means insulatingly mounting said units so that said planes are substantially parallel; means insulatingly connecting said sliders for unitary rotation, from a normal position in which one of said sliders is at one of said rst named points and the other slider is at one of said last named points; means electrically connecting said tap means; means energizing said windings with voltages whose magnitudes are sine and cosine functions of a variable; and voltage responsive means connected between said sliders.

WALDO H. KLIEVER.

References Cited in the le of this patent UNITED STATES PATENTS Number Name Date 2,025,580 Engelhardt Dec. 24, 1935 2,027,393 McCreary Jan. 14, 1936 2,158,500 Guerra May 16, 1939 2,220,055 Fischel et al Oct. 29, 1940 2,261,309 Stuart Nov. 4, 1941 2,287,296 Dallos June 23, 1942 2,346,849 Lear Apr. 18, 1944 2,357,319 Esval et a1 Sept. 5, 1944 2,357,922 Ziebolz et al. Sept. 12, 1944 2,361,433 Stuart Oct. 31, 1944 2,363,500 Carter et al. Nov. 28, 1944 2,392,370 Esval et al. Jan. 8, 1946 2,396,244 Borsum Mar. 12, 1946 2,404,387 Lovell et al. July 23, 1946 2,406,016 Heising Aug. 20, 1946 2,428,747 Zebolz Oct. 7, 1947 2,434,057 lSproule Jan. 6, 1948 2,441,269 Hartig May 11, 1948 2,452,042 Everett et al. Oct. 26, 1948 2,454,184 Kliever Nov. 16, 1948 2,483,125 Cummerow et a1. Sept. 27, 1949 2,491,725 Glass Dec. 20, 1949 2,502,786 Hayslett Apr. 4, 1950 FOREIGN PATENTS Number Country Date 578,784 Great Britain July 11, 1946 OTHER REFERENCES Kliever & 'Syrdal, Cathode-Ray Compass."

Product Engineering, August 1947, pp. 132-134. (Copy Div. 66.)

Kliever & Syrdal, A Magnetic Compass with Cathode-Ray Sensing Element, AIEE Transactions, 1947, vol. 66. pp. 529-534. (Copy Div. 66.) 

